Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations
Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the ele...
Ausführliche Beschreibung
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| Autor*in: |
Bähring, A. [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1985 |
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| Anmerkung: |
© Springer-Verlag 1985 |
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| Übergeordnetes Werk: |
Enthalten in: Zeitschrift für Physik. A, Hadrons and nuclei - Springer-Verlag, 1975, 320(1985), 1 vom: März, Seite 141-149 |
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| Übergeordnetes Werk: |
volume:320 ; year:1985 ; number:1 ; month:03 ; pages:141-149 |
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| DOI / URN: |
10.1007/BF01411934 |
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| 245 | 1 | 0 | |a Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations |
| 264 | 1 | |c 1985 | |
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| 520 | |a Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. | ||
| 650 | 4 | |a Coherence | |
| 650 | 4 | |a Density Matrix | |
| 650 | 4 | |a Collision Energy | |
| 650 | 4 | |a Impact Parameter | |
| 650 | 4 | |a Inelastic Collision | |
| 700 | 1 | |a Meyer, E. |4 aut | |
| 700 | 1 | |a Hertel, I. V. |4 aut | |
| 700 | 1 | |a Schmidt, H. |4 aut | |
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10.1007/BF01411934 doi (DE-627)OLC2029716286 (DE-He213)BF01411934-p DE-627 ger DE-627 rakwb eng 530 VZ Bähring, A. verfasserin aut Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1985 Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. Coherence Density Matrix Collision Energy Impact Parameter Inelastic Collision Meyer, E. aut Hertel, I. V. aut Schmidt, H. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 320(1985), 1 vom: März, Seite 141-149 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:320 year:1985 number:1 month:03 pages:141-149 https://doi.org/10.1007/BF01411934 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 320 1985 1 03 141-149 |
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10.1007/BF01411934 doi (DE-627)OLC2029716286 (DE-He213)BF01411934-p DE-627 ger DE-627 rakwb eng 530 VZ Bähring, A. verfasserin aut Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1985 Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. Coherence Density Matrix Collision Energy Impact Parameter Inelastic Collision Meyer, E. aut Hertel, I. V. aut Schmidt, H. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 320(1985), 1 vom: März, Seite 141-149 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:320 year:1985 number:1 month:03 pages:141-149 https://doi.org/10.1007/BF01411934 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 320 1985 1 03 141-149 |
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10.1007/BF01411934 doi (DE-627)OLC2029716286 (DE-He213)BF01411934-p DE-627 ger DE-627 rakwb eng 530 VZ Bähring, A. verfasserin aut Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1985 Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. Coherence Density Matrix Collision Energy Impact Parameter Inelastic Collision Meyer, E. aut Hertel, I. V. aut Schmidt, H. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 320(1985), 1 vom: März, Seite 141-149 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:320 year:1985 number:1 month:03 pages:141-149 https://doi.org/10.1007/BF01411934 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 320 1985 1 03 141-149 |
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10.1007/BF01411934 doi (DE-627)OLC2029716286 (DE-He213)BF01411934-p DE-627 ger DE-627 rakwb eng 530 VZ Bähring, A. verfasserin aut Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1985 Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. Coherence Density Matrix Collision Energy Impact Parameter Inelastic Collision Meyer, E. aut Hertel, I. V. aut Schmidt, H. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 320(1985), 1 vom: März, Seite 141-149 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:320 year:1985 number:1 month:03 pages:141-149 https://doi.org/10.1007/BF01411934 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 320 1985 1 03 141-149 |
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10.1007/BF01411934 doi (DE-627)OLC2029716286 (DE-He213)BF01411934-p DE-627 ger DE-627 rakwb eng 530 VZ Bähring, A. verfasserin aut Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations 1985 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 1985 Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. Coherence Density Matrix Collision Energy Impact Parameter Inelastic Collision Meyer, E. aut Hertel, I. V. aut Schmidt, H. aut Enthalten in Zeitschrift für Physik. A, Hadrons and nuclei Springer-Verlag, 1975 320(1985), 1 vom: März, Seite 141-149 (DE-627)129415375 (DE-600)189286-1 (DE-576)014793679 0939-7922 nnns volume:320 year:1985 number:1 month:03 pages:141-149 https://doi.org/10.1007/BF01411934 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_20 GBV_ILN_21 GBV_ILN_22 GBV_ILN_24 GBV_ILN_30 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_59 GBV_ILN_62 GBV_ILN_70 GBV_ILN_105 GBV_ILN_130 GBV_ILN_150 GBV_ILN_170 GBV_ILN_2006 GBV_ILN_2010 GBV_ILN_2012 GBV_ILN_2014 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2185 GBV_ILN_2192 GBV_ILN_2221 GBV_ILN_2279 GBV_ILN_2360 GBV_ILN_4012 GBV_ILN_4035 GBV_ILN_4046 GBV_ILN_4082 GBV_ILN_4103 GBV_ILN_4126 GBV_ILN_4277 GBV_ILN_4302 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4310 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4319 GBV_ILN_4323 GBV_ILN_4336 GBV_ILN_4700 AR 320 1985 1 03 141-149 |
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Coherence effects in low energy $ Na^{*} $(3p)+$ Na^{+} $ scattering: Experiment and semiclassical calculations |
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Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. © Springer-Verlag 1985 |
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Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. © Springer-Verlag 1985 |
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Abstract Pronounced polarization effects have been observed in inelastic collisions of laser state-prepared $ Na^{*} $(3p,ML) with $ Na^{+} $ leading to $ Na^{*} $(3d) for the energy rangeECM=20–45 eV. Using linearly polarized light the dependence of the inelastic process on the alignment of the electronic charge cloud of the $ Na^{*} $(3p) prior to the collision has been measured. In studies with left and right hand circularly polarized light the angular momentum transferred in the collision process has been determined. The results are compared with similar data for the 3p→3s deexitation process studied previously [6]. The density matrix of the $ Na^{*} $(3p) state has been evaluated with respect to the collisional excitation to $ Na^{*} $(3d). Semiclassical calculations based on the coupled channel impact parameter approximation using pseudopotentials [7] and nonadiabatic rotational coupling elements for the Na2* system [12] have been performed. The agreement with the experimental results is good, in particular for the higher collision energies. © Springer-Verlag 1985 |
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